Before special relativity, mass and energy were considered separate things in theoretical approaches. The mass-energy relation, E = mc2, is an equation in Albert Einstein’s particular relativity theory that states that mass and energy are the same and that they may be converted into one another. The kinetic energy (E) of a body is equal to its increased relativistic mass (m) times the speed of light squared (c2) in the equation.
The binding energy of nuclei is so high that it accounts for a large portion of their mass.
Because energy is required when the nucleus is created, the mass is always smaller than the sum of the separate masses of the component protons and neutrons. The mass, which is converted into energy, is subtracted from the overall mass of the original particles.
The mass that is converted into energy when the nucleus is produced is represented by the mass defect.
According to the particular theory of relativity, E = mc2 is the relationship between mass and energy. The function of mass is energy. The more mass a body has, the more energy it gains or releases.
The term “mass-energy relation” refers to the fact that mass and energy are the same and may be changed into one another. Einstein proposed this concept. However, he was not the first to do so. With his theory of relativity, he accurately described the relationship between mass and energy. The equation is written as E = mc2 and is known as Einstein’s mass-energy equation.
Where E is the object’s equivalent kinetic energy, m is the object’s mass (Kg), and c is the speed of light (c = 3 x 108 m/s).
Furthermore, the mass-energy relation indicates that the body’s rest mass will drop if energy is released from the body due to such a conversion. Ordinary chemical reactions involve such a transfer of rest energy to other types of energy, while nuclear reactions involve significantly bigger conversions.
Even though a system’s overall mass changes, its total energy and momentum stay constant, according to mass-energy relation. Consider an electron colliding with a proton. Both particles’ mass is destroyed, but a tremendous amount of energy in photons is generated. The concept of the mass-energy equation was influential in developing atomic fusion and fission theories.
Binding Energy
The smallest amount of energy needed to remove a particle from a system of particles is known as Binding Energy. Put another way, it’s the energy used to break down a system of particles into single units. The binding energy term is used to describe energy separation in nuclear physics.
Binding energy is calculated by subtracting the sum of the masses of protons and neutrons from the masses of various nuclei. The energy released during nuclear reactions is calculated using binding energy measurements.
Because all nuclei require net energy to divide them into individual protons and neutrons, the binding energy of nuclei is always positive.
Once the mass defect has been calculated, the nuclear binding energy can be estimated by transforming mass to energy using E = mc2. When you calculate the energy in joules for a nucleus, you can scale it down to per-mole and per-nucleon amounts.
Mass Defect
Given equation describes the relationship between energy and mass:
E = mc2
The speed of light is denoted by c. The binding energy of nuclei is so great that they can hold a lot of mass.
Because energy is required when the nucleus is produced, the actual mass is always smaller than the sum of the atomic masses of the nucleons. This energy is made up of mass, called mass defect, since it is exerted from the overall mass of the initial atom.
𝚫M = (Zmp + Nmn) – MA
M – mass defect
MA – the mass of the nucleus
mp – mass of a proton (1.00728 amu)
mn – the mass of a neutron (1.00867 amu)
Z – number of protons
N – number of neutrons
Binding Energy Calculation
Binding energy calculation can be done in the following way:
Binding Energy = mass defect x c2
where c = speed of light in vacuum
c = 2.9979 x 108 m/s.
Binding Energy is expressed in terms MeV’s/nucleon or kJ/mole of nuclei.
Conclusion:
The amount of energy needed while forming the nucleus, or the mass defect multiplied by the speed of light squared, is equal to the nuclear binding energy (BE). The graph of binding energy per nucleon (BEN) versus atomic number ‘A’ shows that dividing or combining nuclei releases a vast amount of energy.
The ionisation energy of an electron in an atom is equivalent to the binding energy of a nucleon in a nucleus.